{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:NCALDI2FNMEOI5SSSQZ4L4JNYR","short_pith_number":"pith:NCALDI2F","schema_version":"1.0","canonical_sha256":"6880b1a3456b08e476529433c5f12dc4657eb0f70c6032a25e1ef1f1aa5ad36d","source":{"kind":"arxiv","id":"2209.10110","version":2},"attestation_state":"computed","paper":{"title":"Probing the non-standard neutrino interactions using quantum statistics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C. S. Kim, Dibyakrupa Sahoo, Janusz Rosiek","submitted_at":"2022-09-19T18:01:17Z","abstract_excerpt":"Using the well established principles of Lorentz invariance, CP and CPT symmetry, and quantum statistics we do a model-independent study of effects of possible non-standard couplings of (Dirac and Majorana) neutrinos. The study is sensitive to the different quantum statistical properties of the Dirac and Majorana neutrinos which, contrary to neutrino-mediated processes of lepton number violation, could lead to observable effects not suppressed by the small ratios of neutrino and heavier particle masses. For processes with a neutrino-antineutrino pair of the same flavor in the final state, we f"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2209.10110","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-09-19T18:01:17Z","cross_cats_sorted":[],"title_canon_sha256":"db788f80b4d4fea7d44837f27a467e2ce1ea1c171f840a539ebc78ab4aa10d22","abstract_canon_sha256":"cecaae6471cd83fd802372f7e1700c188a2e896bec3f381c53ef71556b8b1e2e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:54:55.147589Z","signature_b64":"yLeDExFLpOvPP8IcAq3o+uVryb+K5nyricjzMJtm0DN3T4I77i3EpwRSFGFdYCAusZc9PAwinvPdD4RIPeBPCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6880b1a3456b08e476529433c5f12dc4657eb0f70c6032a25e1ef1f1aa5ad36d","last_reissued_at":"2026-07-05T05:54:55.147118Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:54:55.147118Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Probing the non-standard neutrino interactions using quantum statistics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C. S. Kim, Dibyakrupa Sahoo, Janusz Rosiek","submitted_at":"2022-09-19T18:01:17Z","abstract_excerpt":"Using the well established principles of Lorentz invariance, CP and CPT symmetry, and quantum statistics we do a model-independent study of effects of possible non-standard couplings of (Dirac and Majorana) neutrinos. The study is sensitive to the different quantum statistical properties of the Dirac and Majorana neutrinos which, contrary to neutrino-mediated processes of lepton number violation, could lead to observable effects not suppressed by the small ratios of neutrino and heavier particle masses. For processes with a neutrino-antineutrino pair of the same flavor in the final state, we f"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2209.10110","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2209.10110/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2209.10110","created_at":"2026-07-05T05:54:55.147177+00:00"},{"alias_kind":"arxiv_version","alias_value":"2209.10110v2","created_at":"2026-07-05T05:54:55.147177+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2209.10110","created_at":"2026-07-05T05:54:55.147177+00:00"},{"alias_kind":"pith_short_12","alias_value":"NCALDI2FNMEO","created_at":"2026-07-05T05:54:55.147177+00:00"},{"alias_kind":"pith_short_16","alias_value":"NCALDI2FNMEOI5SS","created_at":"2026-07-05T05:54:55.147177+00:00"},{"alias_kind":"pith_short_8","alias_value":"NCALDI2F","created_at":"2026-07-05T05:54:55.147177+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.09124","citing_title":"Invisible decays of vector Charmonia and Bottomonia to determine the Weak Mixing Angle at quarkonia scale","ref_index":25,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/NCALDI2FNMEOI5SSSQZ4L4JNYR","json":"https://pith.science/pith/NCALDI2FNMEOI5SSSQZ4L4JNYR.json","graph_json":"https://pith.science/api/pith-number/NCALDI2FNMEOI5SSSQZ4L4JNYR/graph.json","events_json":"https://pith.science/api/pith-number/NCALDI2FNMEOI5SSSQZ4L4JNYR/events.json","paper":"https://pith.science/paper/NCALDI2F"},"agent_actions":{"view_html":"https://pith.science/pith/NCALDI2FNMEOI5SSSQZ4L4JNYR","download_json":"https://pith.science/pith/NCALDI2FNMEOI5SSSQZ4L4JNYR.json","view_paper":"https://pith.science/paper/NCALDI2F","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2209.10110&json=true","fetch_graph":"https://pith.science/api/pith-number/NCALDI2FNMEOI5SSSQZ4L4JNYR/graph.json","fetch_events":"https://pith.science/api/pith-number/NCALDI2FNMEOI5SSSQZ4L4JNYR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NCALDI2FNMEOI5SSSQZ4L4JNYR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NCALDI2FNMEOI5SSSQZ4L4JNYR/action/storage_attestation","attest_author":"https://pith.science/pith/NCALDI2FNMEOI5SSSQZ4L4JNYR/action/author_attestation","sign_citation":"https://pith.science/pith/NCALDI2FNMEOI5SSSQZ4L4JNYR/action/citation_signature","submit_replication":"https://pith.science/pith/NCALDI2FNMEOI5SSSQZ4L4JNYR/action/replication_record"}},"created_at":"2026-07-05T05:54:55.147177+00:00","updated_at":"2026-07-05T05:54:55.147177+00:00"}